All experiments were conducted under a dry Ar gas atmosphere at 973 K in a glove box. Mo, Ni wires and Ni plates were used as working electrodes. A glassy carbon rod was used as a counter electrode. The reference electrode was a Ag wire immersed in a molten CsCl containing 1 mol% of AgCl. All the potentials are referred to the Cs+/Cs electrode potential. The alloy samples were prepared by potentiostatic electrolysis. After electrolysis, the samples were analyzed by XRD and were also observed by SEM-EDS. First, cyclic voltammetry was conducted with a Ni wire electrode in a molten CsCl-DyCl3(0.50 mol%) system. During the cathodic potential scan, a large cathodic current was observed from 0.50 V. Since this potential was more positive than that of Dy metal deposition on a Mo wire electrode, the cathodic current was suggested to correspond to the formation of Dy-Ni alloys. Then, open-circuit potentiometry was carried out with a Mo electrode after electrodepositing Dy metal at 0.11 V for 150 s. A potential plateau was observed at 0.26 V. Since Mo does not form any intermetallic compounds with Dy, the observed potential is interpreted as the Dy3+/Dy potential. Also, open-circuit potentiometry was performed with a Ni electrode after depositing Dy metal at 0.18 V for 90 min. As a result, four potential plateaus were observed at 0.29, 0.42 V, 0.52 V, 0.77 V and 0.90 V, which possibly correspond to the potentials of two-phase coexisting states of different Dy–Ni alloys. Based on these results, potentiostatic electrolysis was conducted at 0.38 V for 1 h with a Ni plate electrode. XRD analysis indicated the formation of DyNi2 on the Ni plate electrode. The thickness of DyNi2 layer was estimated to be 50 μm from cross-sectional SEM observations. The growth rate of this DyNi2 layer, 50 µm h-1, was higher than that obtained in a molten LiCl-KCl system at 700 K, 28 µm h-1 [4]. After the formation of DyNi2 on the Ni plate electrode, potentiostatic electrolysis was also conducted at 0.46 V, 0.66 V and 0.82 V for 1 h. These potential values were selected from the observed plateau potentials. The formed DyNi2 were transformed to other phases such as DyNi3 at 0.46 V, Dy2Ni7 at 0.66 V and DyNi5 at 0.82 V due to anodic dissolution of Dy, depending on the applied potentials.
References
[1] T. Oishi, H. Konishi, T. Nohira, M. Tanaka and T. Usui, Kagaku Kogaku Ronbunshu, 36, 299 (2010). [in Japanese]
[2] H. Konishi, H. Ono, T. Nohira and T. Oishi, ECS Transactions, 50, 463 (2012).
[3] T. Oishi, M. Yaguchi, Y. Katasho, H. Konishi and T. Nohira, J. Electrochem. Soc., 167, 163505 (2020).
[4] H. Konishi, T. Nohira and Y. Ito, Electrochim. Acta, 48, 563 (2003).